Sun Youwen
Chinese Academy of Sciences
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Featured researches published by Sun Youwen.
Plasma Science & Technology | 2009
Qian Jinping; Wan Baonian; L. L. Lao; Shen Biao; S. A. Sabbagh; Sun Youwen; Liu Dongmei; Xiao Bingjia; Ren Qilong; Gong Xianzu; Li Jiangang
Reconstruction of experimental axisymmetric equilibria is an important part of tokamak data analysis. Fourier expansion is applied to reconstruct the vessel current distribution in EFIT code. Benchmarking and testing calculations are performed to evaluate and validate this algorithm. Two cases for circular and non-circular plasma discharges are presented. Fourier expansion used to fit the eddy current is a robust method and the real time EFIT can be introduced to the plasma control system in the coming campaign.
Chinese Physics Letters | 2011
Sun Youwen; Liu Wen-qing; Zeng Yi; Wang Shi-Mei; Huang Shu-hua; Xie Pinhua; Yu Xiao-Man
We demonstrate an effective method to eliminate the interfering effect of water vapor in a non-dispersive infrared multi-gas analyzer. The response coefficients of water vapor at each filter channel are measured from the humidity of the ambient air. Based on the proposed method, the water vapor interference is corrected with the measured response coefficients. By deducting the absorbance of each filter channel related to water vapor, the measuring precision of the analyzer is improved significantly and the concentration retrieval correlation accuracy of each target gas is more than 99%.
Chinese Physics B | 2012
Sun Youwen; Zeng Yi; Liu Wen-qing; Xie Pinhua
In this paper, we present simultaneous multiple pollutant gases (CO2, CO, and NO) measurements by using the non-dispersive infrared (NDIR) technique. A cross-correlation correction method is proposed and used to correct the cross-interferences among the target gases. The calculation of calibration curves is based on least-square fittings with third-order polynomials, and the interference functions are approximated by linear curves. The pure absorbance of each gas is obtained by solving three simultaneous equations using the fitted interference functions. Through the interference correction, the signal created at each filter channel only depends on the absorption of the intended gas. Gas mixture samples with different concentrations of CO2, CO, and NO are pumped into the sample cell for analysis. The results show that the measurement error of each gas is less than 4.5%.
Chinese Physics B | 2012
Chan Ka-Lok; Ling Liuyi; A. Hartl; Zheng Nina; Gerrit Kuhlmann; Qin Min; Sun Youwen; Xie Pinhua; Liu Wen-qing; Mark Wenig
In this paper, we present a comparison of different light-emitting diodes (LEDs) as the light source for long path differential optical absorption spectroscopy (LP-DOAS) atmospheric trace gas measurements. In our study, we use a fiberoptic design, where high power LEDs used as the light source are coupled into the telescope using a Y shape fiber bundle. Two blue and one ultraviolet (UV) LEDs with different emission wavelength ranges are tested for NO2 and SO2 measurements. The detailed description of the instrumental setup, the NO2 and SO2 retrieval procedure, the error analysis, and the preliminary results from the measurements carried out in Science Island, Hefei, Anhui, China are presented. Our first measurement results show that atmospheric NO2 and SO2 have strong temporal variations in that area and that the measurement accuracy is strongly dependent on the visibility conditions. The measured NO2 and SO2 data are compared to the Ozone Monitoring Instrument (OMI) satellite observations. The results show that the OMI NO2 product underestimates the ground level NO2 by 45%, while the OMI SO2 data are highly influenced by clouds and aerosols, which can lead to large biases in the ground level concentrations. During the experiment, the mixing ratios of the atmospheric NO2 and SO2 vary from 8 ppbv to 36 ppbv and from 3 ppbv to 18 ppbv, respectively.
Plasma Science & Technology | 2013
Xu Ming; Wen Yi-Zhi; Xie Jinlin; Yu Chang-Xuan; Gao Bingxi (高炳西); Xu Xiaoyuan; Liu Wandong; Hu Liqun (胡立群); Sun Youwen; Qian Jinping; Wan Baonian
ECE imaging (electron cyclotron emission imaging) is an important diagnostic which can give 2D imaging of temperature fluctuation in the core of tokamak. A method based on ECE imaging is introduced which can give the information of the position of magnetic axis and the structure of internal magnetic surface for EAST tokamak. The EFIT equilibrium reconstruction is not reliable due to the absence of important core diagnostic at the initial phase for EAST, so the information given by ECE imaging could help to improve the accuracy of EFIT equilibrium reconstruction.
Plasma Science & Technology | 2009
Wang Mao; Ding Bojiang; Xu Handong; Zhao Lianmin; Liu Liang; Lin Shiyao; Xu Ping; Sun Youwen; Hu Huaichuan; Yang Yong; Jia Hua; Wang Xiaojie; Wang Dong-xia; Qin Yongliang; Feng Jianqiang; Liu Fukun; Shan Jiafang; Zhao Yanping
An additional lower hybrid wave (LHW) with a higher refractive index (N//) was investigated in the HT-7 tokamak to bridge the spectral gap. It was found that the spectral gap between the wave and the electrons in the outer region was bridged by the additional wave with a higher N// spectrum. The results showed that the sawteeth oscillation was suppressed by launching the additional wave, and that the power deposition profile was moved outwards and the current profile was broadened due to the application of the additional wave. Our study indicates that the spectral gap may be bridged by an additional wave with a higher N// spectrum in the outer region.
Chinese Physics B | 2014
Chen Dalong; Shen Biao; Qian Jinping; Sun Youwen; Liu Guang-jun; Shi Tonghui (石同辉); Zhuang Hui-dong; Xiao Bingjia
Plasma in a typically elongated cross-section tokamak (for example, EAST) is inherently unstable against vertical displacement. When plasma loses the vertical position control, it moves downward or upward, leading to disruption, and a large halo current is generated helically in EAST typically in the scrape-off layer. When flowing into the vacuum vessel through in-vessel components, the halo current will give rise to a large J × B force acting on the vessel and the in-vessel components. In EAST VDE experiment, part of the eddy current is measured in halo sensors, due to the large loop voltage. Primary experimental data demonstrate that the halo current first lands on the outer plate and then flows clockwise, and the analysis of the information indicates that the maximum halo current estimated in EAST is about 0.4 times the plasma current and the maximum value of TPF × Ih/IP0 is 0.65, furthermore Ih/Ip0 and TPF × Ih/Ip0 tend to increase with the increase of Ip0. The test of the strong gas injection system shows good success in increasing the radiated power, which may be effective in reducing the halo current.
Chinese Physics B | 2012
Liu Guang-jun; Wan Baonian; Qian Jinping; Sun Youwen; Xiao Bingjia; Shen Biao; Luo Zhengping; Ji Xiang; Chen Shu-Liang
The effect of passive plates on vertical displacement control in the EAST tokamak is investigated by open loop experiments and numerical simulations based on a rigid displacement model. The experiments and simulations indicate that the vertical instability growth rate is reduced by a factor of about 2 in the presence of the passive plates, where the adjacent segments are not connected to each other. The simulations also show that the vertical instability growth rate is reduced by a factor of about 10 if all adjacent segments on each passive plate loop are connected to each other. The operational window is greatly enlarged with the passive plates. Future tokamaks such as ITER will have an elon- gated cross section, because plasma elongation can im- prove the ratio of tokamak performance-to-cost. How- ever, these plasmas are inherently unstable against vertical displacement. The loss of vertical position control will lead to plasma moving into the vacuum chamber, resulting in disruption and damage to the in- vessel components. Good control of vertical instability is necessary for reliable plasma operation. (1;2) Vertical instability control normally contains two strongly cou- pled parts: the active control and the passive control systems. (3) The active control is realized by external poloidal field (PF) coils, while passive control stems from the stabilizing effect of the conducting structures of the vacuum vessel or built-in vessel components. A passive control system can impede fast vertical dis- placements, while PF coils are used to control slow dis- placement drift. Some of the discharges in tokamaks are out of control because of vertical instability, which is caused by the long response time of the active con- trol system and partially due to relatively weak cou- pling between plasma and active/passive structures. The Experimental Advanced Superconducting Tokamak (EAST) is a full superconducting tokamak with D-shaped cross-section plasma, which is similar to ITERs configuration. There are several reasons for the control of vertical instability to be more difficult on EAST than on a conventional tokamak. Strong coupling between superconducting PF coils and the shielding effects of the in-vessel wall make the response time of the active control system relatively long; the long distance between the PF coils and plasma, due to the thick thermal shielding, relatively weakens their coupling. (4;5) In 2010, a passive plate system was designed and built in EAST to improve the control of vertical in- stability. Compared with an active feedback control system, a passive plate is less expensive and complex, but more sensitive to fast vertical displacement. It can reduce the growth rate of vertical instability and lower the requirements for the response time of the active feedback control system. Stabilization effects of the vacuum vessel on vertical instability have been discussed in Refs. (5) and (6). In this paper, the stabi- lization effect of passive plates on vertical instability is studied by comparing the experimental observation with the numerical simulation based on a rigid dis- placement model, (3;7;8) which has been validated and used in the investigation of vacuum vessel effects on vertical instability. (9) We extend it by including the
Plasma Science & Technology | 2015
Shi Tonghui (石同辉); Wan Baonian; Sun Youwen
In the discharge of EAST tokamak, it is observed that (2,1) neoclassical tearing mode (NTM) is triggered by mode coupling with a (1,1) internal mode. Using singular value decomposition (SVD) method for soft X-ray emission and for electron cyclotron emission (ECE), the coupling spatial structures and coupling process between these two modes are analyzed in detail. The results of SVD for ECE reveal that the phase difference between these two modes equals to zero. This is consistent with the perfect coupling condition. Finally, performing statistical analysis of r1/1, ξ1/1 and w2/1, we find that r1/1 more accurately represents the coupling strength than ξ1/1, and r1/1 is also strongly related to the (2,1) NTM triggering, where r1/1 is the width of (1,1) internal mode, ξ1/1 is the perturbed amplitude of (1,1) internal mode, and w2/1 denot es the magnetic island width of (2,1) NTM.
Chinese Physics B | 2014
Zhang Wei; Hu Liqun; Sun Youwen; Ding Siye; Zhang Zi-Jun; Liu Song-Lin
A peculiar first orbit loss type was found apart from the normal ones when we use ORBIT code to simulate fast ion orbits in the EAST tokamak. Fast ion orbits were studied in the presence of toroidal field (TF) ripple and magnetohydrodynamic (MHD) perturbations. We analyzed the properties of the drifted orbits in detail and compared their differences, finding that the combined effects of ripple and magnetic islands are much greater than the effects of either one of them alone. Then we investigated the orbit deviations as a function of pitch angle in different radial positions. The modeling results demonstrate that the loss of trapped particles is mainly caused by the ripple, while MHD perturbation mainly plays an important role in the passing particles. Furthermore we modeled the loss rate using different equilibriums. Results prove that a higher beta can indeed improve the confinement of fast ions, while a little change in the q profile can make the topologies of magnetic islands become quite different and results in quite different total particle losses.